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12:27 AM
0
Q: Are questions about the field of physics off topic?

M BarbosaI often have questions about the field of physics itself (as opposed to physics questions). For example questions about the current state of a sub-field of physics, or questions about the implications of experiment results. The latter is especially important to me because my knowledge of physics ...

 
 
2 hours later…
2:40 AM
@ACuriousMind Apparently it's a thing to measure mass in pounds
 
user116211
Just giving the definition of the topic doesn't count as a tag wiki, is it so?
 
3:06 AM
@Slereah Did you know that $S^1\times S^1\times S^1$ does not carry a metric of negative curvature
 
3:20 AM
@BernardMeurer so what finally happened to waterloo?
 
@3075 RIP
 
:(
 
Yeah I was pretty sad
 
what did they say?
 
Like someone sent me an email about a week ago saying they needed an outline of my maths course
I said I didn't have that in hand and:
a. asked what would qualify as that and if a signed letter from my principal would do
b. why was it needed since CS didn't ask nor did any other school
they just replied a couple days ago "Hai no openings, kthxbai"
 
3:21 AM
RIP me
 
damn.
 
intro statics problem is kicking my ass
 
@0celo7 Yes. If you're serious about doing engineering you need to be prepared to deal with pounds-mass versus pounds-weight (and in extreme cases kilograms-mass versus kilograms-weight; argh!).
 
@0celo7 electrostatics?
 
@3075 no, statics
 
3:22 AM
@3075 Yeah, sigh
 
did I say electrostatics
 
wow sorry.
i thought you finished first year mechanics.
 
@dmckee kilogram weight???
@3075 no
 
@0celo7 I've seen it. But the metric world has moved much farther along the road to making a clear distinction twixt weight and mass.
 
twixt?
@3075 the picture has an acute angle but I got 270 degrees
 
3:25 AM
nice.
 
@0celo7 Read you Shakespeare, young man. And get off my lawn.
 
So I don't know if the drawing is supposed to show me where I'm supposed to measure the angle from
 
Short for 'betwixt' which means 'between'.
 
Or if it's actually supposed to be acute
@dmckee Owning land is a crime against humanity, old man
 
@3075 Yeah, but my beer is good though
so it's alright I guess
 
3:27 AM
xD
 
Anyway, I'll catch you guys later, hope you're recovering alright @3075
 
thanks, I'm doing ok.
bye.
 
who wants to calc a cross product for me
 
user54412
4:27 AM
LIGO just made a sudden announcement to hold a press conference as part of the American Astronomical Society meeting today/tomorrow, 2016-06-15, 10:15 PDT (17:15 UTC). It will be broadcast here.
 
"JK"
 
user116211
something special?
 
user54412
not sure -- there's excitement in the air
 
user54412
certainly there have been rumors of other signals in the pipeline
 
ALIENS
 
user116211
4:31 AM
ah!
 
6:04 AM
@ChrisWhite A chat session. We need another special chat session for this. It has to be more mergers. @DavidZ @dmckee can we set up a chat session for this?
 
7:04 AM
http://gmwgroup.harvard.edu/research/index.php?page=13

Studying dissipative systems by building them artificially
 
7:38 AM
here you go...another question on the continuity/differentiability of the wavefunction...
3
Q: Can a physical wavefunction be non-smooth (its first derivative is discontinuous)?

IanDsouzaHere's an argument that might support the statement that such a non-smooth wavefunction is not physical: You cannot add a finite number of smooth functions to get a non-smooth function. By fourier expansion theorem, any function can be expressed as a sum of plane waves (which are smooth with res...

this time I couldn't refrain from answering
how did the ama go yesterday?
(it was too late for me here in Japan)
 
 
1 hour later…
user116211
8:53 AM
@yuggib nice to the extent that you can be our next guinea pig ;P
 
@JohnRennie You can set up a chat session, and ask a mod to post an announcement
 
@DavidZ is there any setup needed? I assumed a chat session would just mean us all meeting here at 17:15 UTC.
IIRC that's how it worked for the first LIGO announcement ...
 
user116211
@JohnRennie all in the main page would know about that then if you do that.
 
@JohnRennie I had a sneak preview of this new announcement... ;-P
 
@yuggib Spill,spill!
If an NDA stops you just tell us if we NEED to watch the live stream!!!
 
user116211
8:57 AM
@yuggib don't make suspense ;P
 
user116211
4 hours ago, by Chris White
certainly there have been rumors of other signals in the pipeline
 
there was at least another one
of course it was not confirmed, but I have been told to wait for such an announcement
 
Only one :-(
Still that's enough to make the live stream compulsory
 
well, I know of one
maybe there were more
if they're announcing it probably means they've already another paper accepted
 
@DavidZ: assuming we just meet here at 17:15 UTC, can you make the announcement?
 
9:02 AM
@MAFIA36790 :-D
 
Chris White has added an event to this room's schedule.
 
@MAFIA36790 is there a date already? should I prepare a meta post?
 
@StackExchange Thanks Chris. It never occurred to me to see if I could add the event to the schedule myself.
 
user54412
Hopefully it's something interesting. Given that it's a press conference, and in fact the first press conference since the original, I'm hopeful.
 
I bet on $\geq 2$ new signals
 
user116211
9:07 AM
@yuggib 1st one: no; 2nd one: really don't know; after seeing last night's AMA, I'm sure we can expect further AMAs but of course, no official announcement either. And moreover, it would be too early, i suppose, to write a meta post. I'm waiting for @vzn for further details on that - when the next AMA would happen or so....
 
user54412
Also, I could have been at that meeting, in San Diego no less. Instead I'm working on a paper. I'm not sure if I'm doing grad school quite right.
 
user116211
:(
 
10:15 AM
Is there someone who knows how to use MadGraph to compute partonic cross sections???
Nobody on the internet explains you how to do it without saying a lot of useless details
 
10:45 AM
Are there any exact solutions to string theory?
Like to the Polyakov action
 
@Slereah Uh, it's just the string propagating in a straight line.
 
Hm
What's the gravitational action like in string theory?
 
The "classical" string is a wholly uninteresting object.
 
How do I get pants diagrams
I want a cornucopia of pants
 
@Slereah String theory is an S-matrix theory, not a Lagrangian theory. There is no action.
 
10:54 AM
Oh
How do I get the gravitational S Matrix, then
 
You do get various 10D SUGRA theories as the effective QFTs that produce the tree-level ST results, though
@Slereah You "just" insert the appropriate vertex operator into the string perturbation series.
 
String theory is p. lame
Is there any non-perturbative definition
Also Polchinski defines the string everywhere in his book with a Lagrangian?
 
@Slereah That's the holy grail - but no one has found it yet. Under "M-theory", "F-theory" and other names, various non-perturbative bits are known, but no one knows what the correct non-perturbative formulation of string theory is.
@Slereah You're mistaking the Polyakov action for "the action" of the theory. The defining object of the dynamics of string theory is the string perturbation series/S-matrx.
 
Is there a toy model maybe for string theory?
I dunno, 2+1D strings or something
 
The string theory books are really abysmal at making clear that string theory really is not a QFT
 
10:58 AM
Or are there no non perturbative definition at all
 
@Slereah That's called the "non-critical string" and it's harder than the critical one because there you have the Weyl anomaly hence no clue how to properly quantize
 
Why do people even bother with string theory
 
@Slereah No, we know various things about the non-perturbative formulation provided it exists, but no one knows its proper definition.
 
Do we have clues what it is expected to look like?
 
@Slereah Because it "miraculously" produces many structures that you haven't put in.
@Slereah Yeah, that's what is known as "M-theory"
We know some parts of the spectrum - the BPS objects - for example
But what actual kind of physical theory is might be is probably still open
 
11:03 AM
Is it ghosts
 
Is what ghosts?
 
The real theory
Spooks and haunts
👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻 👻
 
Well, the "M" might stand for "magic" :P
 
Man is there any decent quantum gravity theory
That is both well defined and not proven wrong on some level
 
I think string theory might really be your best bet. It's just very much work in progress, it's as if you had stumbled into QFT before we knew anything about partition functions or path integrals.
That it reproduces QFT at low energy and so generically gives no low energy predictions doesn't help, of course :P
 
11:09 AM
What's the status of Lorentzian gravity, these days
 
I have no idea...I have to go to my string theory class, now
 
Well ask them what the fuck is up
Ask them to make a real theory and stop wasting my time
 
11:52 AM
good morning plebs
> Haradhan Kumar Mohajan
Assistant Professor, Faculty of Business Studies, Premier University, Chittagong,
Bangladesh
GP paper written by a business prof
OK, seems legit
 
12:26 PM
I managed to reference my blog in a PSE answer
 
12:42 PM
@ACuriousMind I told my prof you said a bunch of the stuff I was doing in Milnor and GP can also be done using algebraic topology and he said "where's the fun in that"
 
1:30 PM
Interesting, I knew of a martin who also worked with quantum mechanics
@Martin do you by any chance, studied in UNSW in 2014?
 
::attempts to stalk profs on MO::
 
user116211
1:48 PM
@0celo7 How could it be o.O
 
I meant GR paper of course
 
user116211
yeah... but still... how could it be o.O
 
user116211
a business prof? hmm...
 
user116211
It's nothing but weird ;\
 
@JohnRennie How would you answer this?
Please don't take this the wrong way, but I'd like to see a "low tech" argument
 
user116211
1:52 PM
Have anyone saw Feynman's derivation of Lienard-Wiechard Potential?
 
Never heard of it
 
user116211
It's really giving me a shit.
 
user116211
@0celo7 potentials of a moving charge
 
yeah, that's not a phrase we use in English
@ACuriousMind Are you the second close vote on this?
 
user116211
He used an elementary idea of discrete summation over a point charge dispersed over a cube moving with a non-relativistic velocity.
 
1:55 PM
@0celo7 Yes, I don't know what that question is attempting to do.
If he wants to find out whether a metric is flat, why not just compute the curvature?
 
user116211
But actually he overcounts the charge in the volume slices.
 
@ACuriousMind I'm still not convinced that curvature 0 <==> Euclidean space (locally)
The proof uses the damn black box of black boxes
The Frobenius theorem (PDE version)
 
user116211
There is a PSE post on this... but actually the answer doesn't seem to point the mistake of Feynman.
 
user116211
5
Q: Feynman's proof for Liénard-Wiechert's potential of a moving charge

guillefixFeynman's proof utilizes a geometrical and fundamental integration argument. I like it, except this bit: What makes me unconfortable somehow is that in (c) we are counting in some of the charge we counted at (b). It seems to me that it is this extra counting which makes the potential to be lar...

 
@ACuriousMind You know a black box is bad when it's used to prove other black boxes!
 
1:57 PM
::shrugs::
 
@ACuriousMind what's that shrug for
do you know the proof?
 
@0celo7 The shrug indicates I don't care
 
:/
How can you maintain such an attitude
 
@Secret: No, in fact, I've sadly never been to Australia, yet.
 
Guys, does anyone here knows how to use MadGraph?
 
2:36 PM
@0celo7 What does constant curvature mean in 4D Lorentian manifold. In a 2D Riemannian manifold I'd say it was a constant Gaussian curvature, but I'm unsure how this extends to spacetime.
 
@JohnRennie In this case it means the curvature scalar is constant
 
@0celo7 The Ricci scalar?
 
@JohnRennie yes
Same difference
 
Well I suppose I'd compute the Ricci scalar - actually I'd just Google for the result.
 
@JohnRennie I also believe it follows from Schur's lemma.
you'd probably have to modify it for spacetime
@JohnRennie erm, you don't know the metric yet
this is part of the derivation of it
frick
the idea of sectional curvature doesn't work that well
I know Beem wrote a bunch of papers on it.
because you can have degenerate planes, i.e. planes generated by null vectors
@JohnRennie also do you know what this guy is asking for physics.stackexchange.com/questions/262711/…
 
2:50 PM
is $\mathcal{O}$ a set?
nvm it is
 
@Obliv what?
 
what the hell is that
what kind of question is that
 
it's an equivalence class
called an orbit i think
 
Just writing down a letter and asking if it is a set is not a meaningful question.
Never assume your notation is universally known.
 
@acuriousmind I was going to explain but i realized the answer before i could
 
2:53 PM
@0celo7 I can't see the point of that. Any form of the flat space metric is related to the Minkowksi metric by a coordinate transformation. So the most general form would be written as an arbitrary transformation applied to the Minkwski metric. This strikes me as a boring thing to do.
 
@JohnRennie *locally minkowski
You could have some weird topology
but yes I agree
not sure what OP wants
 
Hey lagrange's theorem : "if $G$ is a finite group and $H$ is a subgroup of $G$, then $|H|$ divides $|G|$" only applies when there is a bijective map $\varphi: H \to \mathcal{O}$? Also, I get that this means $\forall h \in H$, $x = hb$ ,for some $x,b\in G$ so that the elements of $H$ divide the elements in $G$. How does this indicate the cardinality of the subgroup divides the cardinality of the group though?
Sorry if i'm not being clear let me know where I don't make sense
 
3:09 PM
@Obliv You still haven't told us what $\mathcal{O}$ is. Also, Lagrange's theorem always holds.
 
let's try to learn inverse scattering transform again
I want some of that sine gordon
 
$\mathcal{O}$ is the equivalence class of an element $x \in G$ under ~ where ~ is defined as $x$~$b$ if $x = hb$ for some $h \in H$ and $x,b \in G$, $H$ is acting on $G$.
 
Is sine gordon even well defined as a QFT
It has arbitrarily high derivatives
Is it even causal
 
@Obliv sounds like some coset stuff
 
@Obliv Not indicating of which element it is such an equivalence class is poor form (that is, at least write $\mathcal{O}_x$). But, apart from that, what exactly is your question?
 
3:13 PM
@Obliv the best notation is always $[x]$
For instance, I am now classifying the equivalence classes of codimension $p$ Pontryagin manifolds where ~ is framed cobordism
Fun fun
And I'm calling them $[x_i]$
 
@acuriousmind well suppose you have a bijective map $H \to \mathcal{O}_x$ where $H$ is a subgroup of $G$ acting on $G$. $x \in G$. How can this information alone let us deduce that $|H|$ divides $|G|$? I thought the orbit just shows that the elements of the group being acted on is divisible by the group's elements acting on it.
@0celo7 i have no idea what that means. what's a coset?
 
@Obliv I don't know either
 
@Obliv I need not suppose that, the map is simply given by $h\mapsto hx$. This means that all equivalence classes have the same size as $H$. Furthermore all equivalence classes are disjoint (because equivalence classes always are). If $\lvert G \rvert$ is finite, then it's a finite disjoint union (of say $n$ classes), so $\lvert G \rvert = n\lvert H \rvert$.
 
@acuriousmind $H \to \mathcal{O}_x$ maps elements $h \in H$ to the relation $x$~$h$, correct? So this means $h \to x = hx$ so $h \to hx$ I get that part. Doesn't this just mean the equivalence class of $x \in G$ under ~ is the size of $H$? This is only one element of $G$. Is this supposed to be extended to all elements in $G$?
 
@Slereah The worst is translating math into GR
 
3:23 PM
@0celo7: maybe this is a silly question, but does the assumption of homogeneity mean there cannot be an inhomogeneous solution? For example the vacuum is homogeneous, and while we do indeed get a homogeneous solution (Minkowski) we also get inhomogeneous solutions (Schwarzschild, Kerr, etc).
 
especially since GR abuses a lot of math terms
 
@Obliv What does "maps to the relation $x\sim h$" mean? Your second sentence doesn'T make any sense at all to me. But yes, from the existence of a bijection $H\to \mathcal{O}_x$ we conclude that the equivalence class $\mathcal{O}_x$ has size $\lvert H\rvert$, and since nothing was special about $x$, this holds for all elements in $G$, there is nothing to "extend".
 
There's like ten homogeneous vacuum solutions
In 4D
In 2D it's like
Flat space
Cylinder
Other cylinder
Torus
Klein bottle
Other Klein bottle
Projective plane
I think, anyway
Might be a little more
 
@Slereah: is that a reponse to my post?
 
@acuriousmind well the orbit $\mathcal{O}$ is an equivalence class under an equivalence relation. Since the set $\mathcal{O}$ is made of elements that satisfy this relation, I think of it as those elements, which are mapped, having to satisfy this relation. I just wrote it as being mapped to it to save time
 
3:26 PM
somewhat
 
Alright thank you :)
 
I think those are the only homogeneous flat solutions
 
@Slereah I don't see how that answers my question
 
@Obliv I have no idea what you just said.
 
I dunno mang
What is your question exactly
I'm not quite sure
 
3:28 PM
@Slereah There are vaccum solutions that don't have constant curvature even though the vacuum is isotropic and homogeneous. Yes?
 
They have constant curvature
 
@acuriousmind $\mathcal{O}_x = \{a,b,c,...~|~x$~$a\}$, right? So if $H \to \mathcal{O}_x$ then $h \in H$ must satisfy the condition in the set $\mathcal{O}_x$?
 
Well, they are Ricci flat, anyway
 
So I just saved time by saying $h \in H$ was being mapped to $x$~$h$
 
@Slereah The Kretschmann scalar is not constant e.g. in the Schwarzschild metric
 
3:29 PM
If you mean the Riemann tensor, then yes, you can have vacuum solutions that are not flat
 
People often said quantum states are vectors in hilbert space, but why there isn't any states that acts like the zero vector, i.e. when superimposed onto another state, does not change the state?
 
That's because in >2+1D, the Riemann tensor does not depend exclusively on the Ricci tensor
The 0 vector doesn't have norm 1
Quantum states are rays
0 is not a ray
 
@Obliv "What?" to the first question. "If $H\to\mathcal{O}_x$" doesn't make any sense,$A\to B$ is not a statement, and no, if $h\sim x$ for some $h\in H$, then $\mathcal{O}_x$ is the equivalence class of the identity.
You have to be way more careful with the way you state things in math.
 
@Slereah So can we have solutions for an isotropic and homogeneous non-vacuum solution that do not have constant curvature? i.e. the various scalars are not constants.
 
Sure
The De Sitter Schwarzschild solution, for instance
Wait, no, it's not homogeneous
Wait if it's isotropic and homogeneous and non vacuum
It's gonna be either dS or AdS
 
3:32 PM
@Slereah why?
 
Well you can check it by hand
Apply all the Killing vectors
 
The vacuum can be Minkwski, or Schwarzschild or Kerr or etc etc
 
You'll find out that the Riemann tensor is entirely determined by a scalar
But Schwarzschild isn't homogeneous
 
Why if you add a small constant energy density is the FLRW metric the only solution?
 
$r$ isn't a Killing vector at all
 
3:34 PM
@acuriousmind by definition if the set $H$ is being mapped to a set that imposes a condition, the elements in the set $H$ must satisfy this condition in order for this to be a bijection, right? Also $H \to \mathcal{O}_x$ is supposed to signify mapping of $H$ to $\mathcal{O}$. Lastly, $h$~$x$ must be true in order for the $h$ to be in the orbit of $x$ I thought
 
@Obliv nononononono. You can map the odd numbers to the even numbers by adding 1. That doesn't mean that odd numbers satisfy the condition of being even.
 
Suppose you make the stress-energy tensor diag(e,0,0,0) for some small constant e. In the limit of e=0 we get all the vacuum solutions. For non-zero but infinitesimally small e the only solution is FLRW. Is that correct?
 
And I know that $H\to\mathcal{O}$ is supposed to "signify a mapping", it's just that "If $A\to B$" is not a meaningful statement. "If $f:A\to B$ exists" or "If $f:A\to B$ is a bijection" works, but "If $A\to B$" just doesn't mean anything.
 
Errrr maybe?
 
Insufficient effort?
0
Q: What is the volume of a 4d sphere

DaMegaBoss99What is the volume of a 4d sphere? I've seen so many site that would have answered this question, but all of them have so many numbers that some people (including me) don't understand. So I was hoping somebody here would give me a nice simple explanation.

 
3:39 PM
Constant dust solution would be FRLW I think yeah
 
@JohnRennie Not about physics, homework-like question, no effort, take your pick :P
 
Wait.. so $f: H\to \mathcal{O}_x$ is a bijection isn't implying that $x$~$h$ for all $h \in H$? So there is no significance in $\mathcal{O}_x$'s relation being $x$~$h$ iff $x = hb$ as long as it's an equivalence relation and this map $f$ is a bijection, $|H|$ divides $|G|$? I feel stupid now @acuriousmind
 
@Obliv I'll state this once again properly: The bijection is given by $f : H\to\mathcal{O}_x, h \mapsto f(h)=hx$ (prove that this is a bijection!). This means that $\lvert \mathcal{O}_x\rvert = \lvert H \rvert$ for all $x\in G$. Since $G$ is the disjoint union of $n$ such equivalence classes, $\lvert G\rvert = n\lvert H \rvert$.
Don't try anything else until you have understood this argument.
 
@Slereah well yes. When I started thinking about it maybe was the best I could come up with as well.
 
so a little bird told me I should watch the new gravity wave conference today
 
3:45 PM
@GPhys Absolutely, more merger detections!! (Allegedly :-)
Though it doesn't start for 90 minutes yet.
 
Pretty sure that all tensor fields related to the metric are identical for a homogeneous and isotropic spacetime, though
 
fun
 
@Slereah and yet the vacuum is homogeneous and isotropic ...
 
What I'm about to say might sound really stupid and you might get mad at me @acuriousmind but I must say it. It's a bijection because by definition $f(h) = (x,h) \in \mathcal{O}_x = x$~$h = hx$ and all of the domain $H$ is being mapped to the equivalence class so all $h\in H$ map to $hx$. What's wrong with this reasoning?
 
@JohnRennie No
There are plenty of vacuum solutions which are not
 
3:51 PM
You misunderstand me. In a vaccum the stress-energy tensor is isotropic and homogeneous, and in an FLRW spacetime the stress-energy tensor is isotropic and homogeneous. So why are there many vacuum solutions and only one FLRW metric?
 
Oh, you mean the stress energy tensor
Hm
Also when you say "isotropic and homogeneous", you mean just the spatial part, right?
 
@Slereah yes
 
I'd say there are more than one solution type for the same homogeneous and isotropic stress energy tensor
Symmetries of the SET are symmetries of the Ricci tensor
Those will only determine the Ricci tensor
The Weyl tensor is still free
 
hello
 
@KISHORE_ZE Hi. Come for the gravity wave chat?
 
3:56 PM
I suppose
LIGO Gravity WAve lab press conf.
 
@Obliv I have no idea what $f(h)=(x,h)\in\mathcal{O}_x = x\sim h = hx$ is supposed to mean, and I don't understand your reasoning at all. What is $(x,h)$?! Why is it $f(h)$, or an element of $\mathcal{O}_x$.
 
Wave*
I'm new to stack physics
why dosen't the formatting show up for me?
 
@JohnRennie the assumption of homogeneity is cosmology
Schwarzschild is not a cosmological model
 
@KISHORE_ZE Mathjax isn't supported in the chat by default.
 
@ACuriousMind damn you're pretty harsh
 
3:58 PM
Oh
Thanks
 
@JohnRennie homogeneous basically means that you can find coordinates in which the metric components are constant
@JohnDuffield still does not understand this
 
He's not talking about symmetries of the metric tho
Only of the SET
 
@Slereah Yes!!! (SET = stress-energy tensor)
 
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